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NSR database version of April 11, 2024.

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2007FR11      Phys.Rev. C 75, 065802 (2007)

R.H.France III, E.L.Wilds, J.E.McDonald, M.Gai

Further measurement of the β-delayed α-particle emission of 16N

RADIOACTIVITY 16N(β-); measured delayed α spectrum. Compared results to existing data.

doi: 10.1103/PhysRevC.75.065802
Citations: PlumX Metrics


2007WI09      Phys.Rev. C 76, 018501 (2007)

E.L.Wilds, Jr., R.H.France III, J.E.McDonald, Z.Zhao, M.Gai

Upper limits on the first-forbidden rank-one β decay of 20F

RADIOACTIVITY 20F(β-); measured Eβ, Eγ, Eα. Deduced first forbidden decay branching ratios.

doi: 10.1103/PhysRevC.76.018501
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2003FR22      Nucl.Phys. A718, 398c (2003)

R.H.France III, L.T.Baby, C.Bordeanu, Th.Delbar, J.A.Dooley, M.Gai, M.Hass, J.E.McDonald, A.Ninane, C.M.Przybycien

Destruction of 7Li and 7Be in astrophysical environments

NUCLEAR REACTIONS 7Li(3He, α), (3He, d), E=390-1130 keV; measured Eα, σ, σ(θ).

doi: 10.1016/S0375-9474(03)00813-3
Citations: PlumX Metrics


2002MC09      Nucl.Phys. B(Proc.Supp.) S112, 226 (2002)

K.S.McFarland, G.P.Zeller, T.Adams, A.Alton, S.Avvakumov, L.de Barbaro, P.de Barbaro, R.H.Bernstein, A.Bodek, T.Bolton, J.Brau, D.Buchholz, H.Budd, L.Bugel, J.Conrad, R.B.Drucker, B.T.Fleming, R.Frey, J.A.Formaggio, J.Goldman, M.Goncharov, D.A.Harris, R.A.Johnson, J.H.Kim, S.Koutsoliotas, M.J.Lamm, W.Marsh, D.Mason, J.McDonald, C.McNulty, D.Naples, P.Nienaber, V.Radescu, A.Romosan, W.K.Sakumoto, H.Schellman, M.H.Shaevitz, P.Spentzouris, E.G.Stern, N.Suwonjandee, M.Tzanov, M.Vakili, A.Vaitaitis, U.K.Yang, J.Yu, E.D.Zimmerman

Nuclear Effects and the NuTeV sin2θw Measurement

NUCLEAR REACTIONS Fe(ν, X), (ν-bar, X), E not given; measured ratio of neutral to charged-current σ; deduced electroweak parameter, possible nuclear effects on parton distribution functions. Comparison with model predictions.

doi: 10.1016/S0920-5632(02)01777-2
Citations: PlumX Metrics


2002ZE02      Phys.Rev.Lett. 88, 091802 (2002); Erratum Phys.Rev.Lett. 90, 239902(2003)

G.P.Zeller, K.S.McFarland, T.Adams, A.Alton, S.Avvakumov, L.de Barbaro, P.de Barbaro, R.H.Bernstein, A.Bodek, T.Bolton, J.Brau, D.Buchholz, H.Budd, L.Bugel, J.Conrad, R.B.Drucker, B.T.Fleming, R.Frey, J.A.Formaggio, J.Goldman, M.Goncharov, D.A.Harris, R.A.Johnson, J.H.Kim, S.Koutsoliotas, M.J.Lamm, W.Marsh, D.Mason, J.McDonald, C.McNulty, D.Naples, P.Nienaber, A.Romosan, W.K.Sakumoto, H.Schellman, M.H.Shaevitz, P.Spentzouris, E.G.Stern, N.Suwonjandee, M.Tzanov, M.Vakili, A.Vaitaitis, U.K.Yang, J.Yu.E.D.Zimmerman

Precise Determination of Electroweak Parameters in Neutrino-Nucleon Scattering

NUCLEAR REACTIONS 1H(ν, ν'), (ν-bar, ν-bar'), E not given; measured ratio of neutral to charged current σ; deduced electroweak parameter. Comparison with model prediction.

doi: 10.1103/PhysRevLett.88.091802
Citations: PlumX Metrics


2002ZE05      Phys.Rev. D65, 111103 (2002)

G.P.Zeller, K.S.McFarland, T.Adams, A.Alton, S.Avvakumov, L.de Barbaro, P.de Barbaro, R.H.Bernstein, A.Bodek, T.Bolton, J.Brau, D.Buchholz, H.Budd, L.Bugel, J.Conrad, R.B.Drucker, B.T.Fleming, R.Frey, J.A.Formaggio, J.Goldman, M.Goncharov, D.A.Harris, R.A.Johnson, J.H.Kim, S.Koutsoliotas, M.J.Lamm, W.Marsh, D.Mason, J.McDonald, C.McNulty, D.Naples, P.Nienaber, A.Romosan, W.K.Sakumoto, H.Schellman, M.H.Shaevitz, P.Spentzouris, E.G.Stern, N.Suwonjandee, M.Tzanov, M.Vakili, A.Vaitaitis, U.K.Yang, J.Yu, E.D.Zimmerman

Effect of Asymmetric Strange Seas and Isospin-Violating Parton Distribution Functions on sin2θW Measured in the NuTeV Experiment

doi: 10.1103/PhysRevD.65.111103
Citations: PlumX Metrics


2001AL24      Phys.Rev. D64, 012002 (2001)

A.Alton, T.Adams, T.Bolton, J.Goldman, M.Goncharov, R.A.Johnson, N.Suwonjandee, M.Vakili, J.Conrad, B.T.Fleming, J.Formaggio, J.H.Kim, S.Koutsoliotas, C.McNulty, A.Romosan, M.H.Shaevitz, P.Spentzouris, E.G.Stern, A.Vaitaitis, E.D.Zimmerman, R.H.Bernstein, L.Bugel, M.J.Lamm, W.Marsh, P.Nienaber, J.Yu, L.de Barbaro, D.Buchholz, H.Schellman, G.P.Zeller, J.Brau, R.B.Drucker, R.Frey, D.Mason, J.McDonald, D.Naples, S.Avvakumov, P.de Barbaro, A.Bodek, H.Budd, D.A.Harris, K.S.McFarland, W.K.Sakumoto, U.K.Yang

Observation of Neutral Current Charm Production in νμ Fe Scattering at the Fermilab Tevatron

NUCLEAR REACTIONS Fe(ν, X), E ≈ 154 GeV; 1n, 1H(p, X), E(cm)=38.8 GeV; measured charm production σ.

doi: 10.1103/PhysRevD.64.012002
Citations: PlumX Metrics


2001GO43      Phys.Rev. D64, 112006 (2001)

M.Goncharov, T.Adams, A.Alton, T.Bolton, J.Goldman, P.Spentzouris, J.Conrad, B.T.Fleming, J.Formaggio, S.Koutsoliotas, J.H.Kim, C.McNulty, A.Romosan, M.H.Shaevitz, E.G.Stern, A.Vaitaitis, E.D.Zimmerman, R.A.Johnson, M.Vakili, N.Suwonjandee, R.H.Bernstein, L.Bugel, M.J.Lamm, W.Marsh, P.Nienaber, J.Yu, L.de Barbaro, D.Buchholz, H.Schellman, G.P.Zeller, J.Brau, R.B.Drucker, R.Frey, D.Mason, J.E.McDonald, D.Naples, M.Tzanov, S.Avvakumov, P.de Barbaro, A.Bodek, H.Budd, D.A.Harris, K.S.McFarland, W.K.Sakumoto, U.K.Yang

Precise Measurement of Dimuon Production Cross Sections in νμFe and (ν-bar)mFe Deep Inelastic Scattering at the Fermilab Tevatron

NUCLEAR REACTIONS Fe(ν, μ+μ-X), (ν-bar, μ+μ-X), E ≈ 80-270 GeV; measured dimuon production σ. Comparison with previous results.

doi: 10.1103/PhysRevD.64.112006
Citations: PlumX Metrics


1997FR12      Nucl.Phys. A621, 165c (1997)

R.H.France III, E.L.Wildes, N.B.Jevtic, J.E.McDonald, M.Gai

Further Measurement of the Beta-Delayed Alpha-Particle Emission of 16N

RADIOACTIVITY 16N(β-) [from 2H(15N, X), E=70 MeV]; measured β-delayed α spectra. Other data, theory compared.

doi: 10.1016/S0375-9474(97)00231-5
Citations: PlumX Metrics


1996BR37      Phys.Rev. A53, 2194 (1996)

J.-P.Briand, B.d'Etat-Ban, D.Schneider, M.A.Briere, V.Decaux, J.W.McDonald, S.Bardin

Time for the Empty L Shell of a Hollow Atom to be Filled

doi: 10.1103/PhysRevA.53.2194
Citations: PlumX Metrics


1992HI01      Phys.Rev. C45, 601 (1992)

N.M.Hintz, X.H.Yang, M.Gazzaly, S.J.Seestrom-Morris, C.L.Morris, D.C.Cook, A.M.Mack, J.W.McDonald, S.Mordechai, D.S.Oakley, C.F.Moore, M.Lynker, J.D.Zumbro

Determination of Neutron and Proton Multipole Matrix Elements in 208Pb from π- and π+ Scattering at 180 MeV

NUCLEAR REACTIONS 208Pb(π+, π+), (π+, π+'), (π-, π-'), (π-, π-), E=180 MeV; measured σ(θ). 208Pb levels deduced neutron, proton multipole matrix elements.

doi: 10.1103/PhysRevC.45.601
Citations: PlumX Metrics


1992JO03      Phys.Rev. C46, 52 (1992)

M.K.Jones, D.Dehnhard, S.K.Nanda, S.M.Sterbenz, C.L.Morris, M.Plum, J.D.Zumbro, A.H.Hussein, D.S.Oakley, M.J.Smithson, A.L.Williams, J.McDonald, M.A.Bryan, A.H.Fuentes, M.Lynker, D.Crockett, M.A.Machuca, S.Mordechai, C.F.Moore

4He(π, π'p)3H Reaction Near the P33 π-Nucleon Resonance

NUCLEAR REACTIONS 4He(π+, π+'p), (π-, π-'p), E=140, 180 MeV; measured σ(θ(π'), σ(p)) vs excitation energy; deduced reaction mechanisms.

doi: 10.1103/PhysRevC.46.52
Citations: PlumX Metrics


1991MO15      Phys.Rev. C44, 2209 (1991)

C.F.Moore, K.Johnson, G.P.Kahrimanis, J.McDonald, M.Snell, H.J.Ward, S.H.Yoo, C.L.Morris, S.Mordechai, M.Burlein, N.Claytor, H.T.Fortune, R.Ivie, G.B.Liu, J.M.O'Donnell, D.Smith, N.Auerbach, D.Robson

Angular Distributions for the Double Isobaric Analog and a T (<) State at High Excitation in Pion Double Charge Exchange on 93Nb

NUCLEAR REACTIONS 93Nb(π+, π-), E=295 MeV; measured σ(θ(π), E(π)), σ(θ). 93Tc deduced large probability for T< excitation.

doi: 10.1103/PhysRevC.44.2209
Citations: PlumX Metrics


1991OA01      Phys.Rev. C44, 2058 (1991)

D.S.Oakley, R.J.Peterson, S.J.Seestrom, C.L.Morris, M.A.Plum, J.D.Zumbro, A.L.Williams, M.A.Bryan, J.W.McDonald, C.F.Moore

Energy Dependence of Pion Inelastic Scattering from 208Pb

NUCLEAR REACTIONS 208Pb(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=120, 250 MeV; calculated σ(θ). 208Pb levels deduced proton, neutron matrix elements ratio. Different structure models.

doi: 10.1103/PhysRevC.44.2058
Citations: PlumX Metrics


1991WA04      Phys.Rev. C43, 1318 (1991)

D.L.Watson, R.Gilman, C.L.Morris, J.D.Zumbro, S.Mordechai, M.Burlein, J.M.O'Donnell, H.T.Fortune, A.Kotwal, J.Puttz, J.D.Silk, J.S.McDonald, C.F.Moore, A.L.Williams, S.Y.Yoo

Pion-Induced Double Charge Exchange on 12C, 24Mg, 32S, and 40Ca

NUCLEAR REACTIONS 12C, 24Mg, 32S, 40Ca(π+, π-), E=164 MeV; measured σ(θ). Isobar-nucleon interaction mechanism.

doi: 10.1103/PhysRevC.43.1318
Citations: PlumX Metrics


1990JO04      Phys.Rev. C42, R807 (1990)

M.K.Jones, D.Dehnhard, S.K.Nanda, S.M.Sterbenz, C.L.Morris, M.Plum, J.D.Zumbro, A.Hussein, D.S.Oakley, M.J.Smithson, A.L.Williams, J.McDonald, M.A.Bryan, A.H.Fuentes, M.Lynker, D.Crockett, M.A.Machuca, S.Mordechai, C.F.Moore

4He(π, π'p)3H Reaction: Quasifree and resonance scattering

NUCLEAR REACTIONS 4He(π+, π+'p), (π-, π-'p), E=180 MeV; measured σ(θ(π), θp); deduced σ(π+)/σ(π-). DWIA calculation.

doi: 10.1103/PhysRevC.42.R807
Citations: PlumX Metrics


1988AS04      Phys.Lett. 215B, 41 (1988)

D.Ashery, J.Lichtenstadt, E.Piasetzky, C.L.Morris, J.D.Zumbro, R.Gilman, M.W.Rawool, S.Mordechai, B.Boyer, A.Fuentes, K.Johnson, J.W.McDonald, M.J.Smithson, A.Williams, S.H.Yoo, C.F.Moore

A Search for πNN Bound Systems

NUCLEAR REACTIONS 2H(π+, π-), (π-, π+), E=260 MeV; measured possible (πNN) system mass; deduced σ upper limit.

doi: 10.1016/0370-2693(88)91066-0
Citations: PlumX Metrics


1988OA03      Phys.Rev. C38, 2978 (1988)

D.S.Oakley, R.J.Peterson, D.J.Rilett, C.L.Morris, S.J.Greene, B.Boyer, K.Johnson, A.H.Fuentes, J.W.McDonald, M.J.Smithson, A.L.Williams, S.H.Yoo, C.F.Moore

Energy Dependence of Pion Inelastic Scattering to the 1+ States in 12C

NUCLEAR REACTIONS 12C(π-, π-'), (π+, π+'), E=80-295 MeV; measured σ(θ); deduced isobar excitation role. 12C levels deduced σ ratio.

doi: 10.1103/PhysRevC.38.2978
Citations: PlumX Metrics


1987DH01      Phys.Rev. C35, 1148 (1987)

K.S.Dhuga, G.R.Burleson, J.A.Faucett, R.L.Boudrie, W.B.Cottingame, S.J.Greene, C.L.Morris, Z.F.Wang, J.W.McDonald, C.F.Moore, S.Mordechai, A.L.Williams, P.A.Seidl, M.A.Bryan, S.Nanda, S.J.Seestrom-Morris, J.D.Zumbro

Sensitivity of Large-Angle Pion Elastic Scattering to Medium Modifications

NUCLEAR REACTIONS 12C, 16O(π+, π+), E=100-240 MeV; measured σ(θ); deduced model parameter modifications. Optical model.

doi: 10.1103/PhysRevC.35.1148
Citations: PlumX Metrics


1976FO10      Nucl.Phys. A267, 317 (1976)

B.Fogelberg, Y.Kawase, J.McDonald, A.Backlin

Levels in 117Cd Studied in the Decays of 117Ag and 117mAg

RADIOACTIVITY 117Ag [from 235U(n, F)]; measured T1/2, Eγ, Iγ, I(ce), γγ-coin, γγ-delay; deduced ICC, log ft. 117Cd deduced levels, J, π, T1/2, γ-multipolarity, B(E1), B(E2), B(M1). Mass separated fission product. Ge(Li), Si(Li), NaI, plastic detectors.

doi: 10.1016/0375-9474(76)90663-1
Citations: PlumX Metrics


1976MC06      Atomkernenergie 27, 112 (1976)

J.McDonald, N.G.Sjostrand

Measurement of Thermal Neutron Cross Sections for Charged Particle Reactions in Ni59 and Ni61

NUCLEAR REACTIONS 59,61Ni(n, α), 59Ni(n, p), E=thermal; measured σ.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20433.


1975BR07      Phys.Rev. C11, 1122 (1975)

B.A.Brown, D.B.Fossan, J.M.McDonald, K.A.Snover

Recoil-Distance Lifetime Measurements of 48V Levels

NUCLEAR REACTIONS 45Sc(α, nγ), E=9.5 MeV; measured nγ-coin, recoil distance. 48V deduced levels, π, T1/2, B(λ).

doi: 10.1103/PhysRevC.11.1122
Citations: PlumX Metrics


1975KA09      Nucl.Phys. A241, 237 (1975)

Y.Kawase, B.Fogelberg, J.McDonald, A.Backlin

States in 119Cd Studied in the Decay of 119Ag

RADIOACTIVITY 119Ag [from 235U(n, F)]; measured T1/2, Eγ, Iγ, I(ce), γγ-coin, γγ-delay; deduced ICC, log ft. 119Cd deduced levels, J, π, T1/2, γ-multipolarity, B(E1), B(E2), B(M1). Mass separated fission product. Ge(Li), Si(Li), NaI, plastic detectors.

doi: 10.1016/0375-9474(75)90315-2
Citations: PlumX Metrics


1974BR04      Phys.Rev. C9, 1033 (1974)

B.A.Brown, D.B.Fossan, J.M.McDonald, K.A.Snover

Lifetime Measurements and E2 Effective Charges for Nuclei in the 1f7/2 Shell

NUCLEAR REACTIONS 39K(α, n), E=10.4 MeV; 16O, 40Ca(3He, p), E=10.5 MeV; 40Ca, 41K(α, p), E=14.0 MeV; 45Sc(α, p), E=10.0 MeV; 46Ti(α, p), E=11.0 MeV; 40Ca(16O, 2pα), E=47 MeV; 49Ti(α, n), E=14.5 MeV; 40Ca(16O, 3p), E=47 MeV; 40Ca(16O, 2p), E=47 MeV; measured recoil distance. 18F, 42,43Sc, 44Ca, 48Ti, 49V, 50,52Cr, 51,53Mn levels deduced T1/2, B(E2). Deduced 40 < A < 56 effective charges. Natural, enriched targets, Ge(Li) detector.

doi: 10.1103/PhysRevC.9.1033
Citations: PlumX Metrics


1974MC09      Nucl.Phys. A224, 13 (1974); Erratum Nucl.Phys. A239, 530 (1975)

J.McDonald, B.Fogelberg, A.Backlin, Y.Kawase

The Decays of 2.6 min 119gCd and 1.9 min 119mCd to 119In

RADIOACTIVITY 119gCd, 119mCd [from 235U(n, F)]; measured T1/2, Eγ, Iγ, E(ce), I(ce), γγ coin, βγ, γγ delay, deduced multipolarities. 119In deduced levels, J, π, B(E1), B(E2). Isotopically separated 119Cd sources. Ge(Li), Si(Li), NaI(Tl), plastic detectors. Ge(Li)-Ge(Li) coin.

doi: 10.1016/0375-9474(74)90159-6
Citations: PlumX Metrics


1973KE21      Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1822 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.9, 28 (1974)

A.Kerek, P.Carle, J.McDonald

130Te Levels Excited in the β Decay of 130Sb (T1/2 = 40 min)

RADIOACTIVITY 130Sb [from 235U(n, F), isotope separator]; measured Eγ, Iγ, γγ(t). 130Te deduced levels, J, π, T1/2, B(λ).


1973KE23      Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1617 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.8, 48 (1974)

A.Kerek, G.B.Holm, P.Carle, J.McDonald

132Sb States of the Proton-Neutron Hole Type Populated in the Decay of The Doubly Magic Nucleus 132Sn

RADIOACTIVITY 132Sn; measured Eβ, βγ(t), deduced log ft. 132Sb deduced levels, T1/2, J, π. On-line mass separator.


1973KE25      Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1622 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.8, 53 (1974)

A.Kerek, P.Carle, S.Borg, J.McDonald

The 132Sb → 132Te Decay with T1/2 = 3.4 and 4.9 min

RADIOACTIVITY 132Sb; measured βγ(t). Eγ, Iγ, γγ-coin, T1/2, I(ce). 132Te deduced levels T1/2, J, π. On-line mass separator.


1973MC09      Nucl.Phys. A206, 417 (1973)

J.McDonald, A.Kerek

Transition Probability Measurements in 132Te; The Systematics of E2 Transition Rates in Neutron-Rich Even Te Nuclei

RADIOACTIVITY 132Sb [from 235U fission]; measured βγ-, γγ-delay, Eγ, ICC, Iγ. 132Te deduced T1/2, ICC, B(E2). Isotopically separated source. Ge(Li), Si(Li), NaI(Tl), plastic detectors.

doi: 10.1016/0375-9474(73)90544-7
Citations: PlumX Metrics


1972KE20      Nucl.Phys. A195, 159 (1972)

A.Kerek, G.B.Holm, P.Carle, J.McDonald

Proton-Neutron-Hole States in 132Sb Populated in the β-Decay of the Doubly Closed Shell Nucleus 132Sn

RADIOACTIVITY 132Sn[from 235U fission]; measured T1/2, Eγ, Iγ, E(ce), I(ce), Eβ, βγ-coin, γγ-coin, βγ-delay; deduced log ft, Q. 132Sb deduced levels, J, π, T1/2, ICC, B(M1), B(E2), γ-multipolarity. Isotopically separated source;Ge(Li), Si(Li), NaI(Tl), plastic, anthracene detectors, Ge(Li)-Ge(Li) coin.

doi: 10.1016/0375-9474(72)90728-2
Citations: PlumX Metrics


1972KE28      Nucl.Phys. A198, 466 (1972)

A.Kerek, P.Carle, J.McDonald

Properties of 130Te as Observed in the 40 min β-Decay of 130Sb

RADIOACTIVITY 130Sb[from 235U fission]; measured Eγ, Iγ, E(ce), I(ce), Eβ-, γγ-coin, βγ-, γγ-delay; deduced Q. 130Te deduced levels, J, π, ICC, T1/2, B(E2). Isotopically separated source, Ge(Li), Si(Li), NaI(Tl), plastic, anthracene detectors, Ge(Li)-Ge(Li) coin.

doi: 10.1016/0375-9474(72)90702-6
Citations: PlumX Metrics


1972MA67      Phys.Rev. C6, 2109 (1972)

M.Marmor, J.M.McDonald, D.B.Fossan

Lifetime of the 2+ 1759-keV State in 26Al via the 23Na(α, nγ)26Al Reaction

NUCLEAR REACTIONS 23Na(α, nγ), E=9.5 MeV; measured recoil distance. 26Al level deduced T1/2.

doi: 10.1103/PhysRevC.6.2109
Citations: PlumX Metrics


1972MC04      Priv.Comm. (January 1972)

J.McDonald


1972MC09      Phys.Rev.Lett. 28, 1057 (1972)

J.M.McDonald, P.M.S.Lesser, D.B.Fossan

Time-Differential Quadrupole Interactions Following Recoil Implantation

NUCLEAR REACTIONS 111Cd(16O, 16O'γ), E=40 MeV; measured (16O')(γ)(θ, t) in Cd metal; deduced quadrupole interaction frequencies.

doi: 10.1103/PhysRevLett.28.1057
Citations: PlumX Metrics


1971CO08      Phys.Rev. C3, 1352 (1971)

S.Cochavi, J.M.McDonald, D.B.Fossan

Experimental Study of Electromagnetic Matrix Elements in 92Mo

RADIOACTIVITY 92mTc; measured γγ-delay. 92Mo level deduced T1/2. 90Zr(α, 2nγ), E=20-24 MeV; measured σ(E;Eγ), αγ-delay, αγ(θ, H, t). 92Mo(p, p'γ), E=6-9 MeV; measured σ(E;Ep', Eγ), p'γ-delay. 92Mo levels deduced T1/2, μ.

doi: 10.1103/PhysRevC.3.1352
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1971LE24      Nucl.Phys. A170, 663 (1971)

K.W.D.Ledingham, J.Y.Gourlay, J.L.Campbell, M.L.Fitzpatrick, J.G.Lynch, J.McDonald

The Ratio of K-Capture to Positon Emission in the Decay of 30P

RADIOACTIVITY 30P[from 31P(γ, n)]; measured K/β+ ratio.

doi: 10.1016/0375-9474(71)90244-2
Citations: PlumX Metrics


1971MC02      Nucl.Phys. A162, 365 (1971)

J.McDonald, A.Backlin, S.G.Malmskog

Transition Probabilities in 99Tc

RADIOACTIVITY 99Mo[from 98Mo(n, γ)]; measured I(ce), γce-, cece-delay. 99Tc deduced T1/2, ICC, Iγ, mixing ratios, B(E2), B(M1). Enriched target.

doi: 10.1016/0375-9474(71)90991-2
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1971MC10      Nucl.Phys. A176, 526 (1971); Priv. Comm.

J.McDonald, S.G.Malmskog

Levels in 128Te

doi: 10.1016/0375-9474(71)90934-1
Citations: PlumX Metrics


1971SN01      Phys.Rev. C4, 398 (1971)

K.A.Snover, J.M.McDonald, D.B.Fossan, E.K.Warburton

Gamma-Ray Decay of the Low-Lying Levels of Cl34

NUCLEAR REACTIONS 32S(3He, pγ), E=6.8 MeV; measured Eγ, Iγ, Doppler shift attenuation. 31P(α, nγ), E=8-11 MeV; measured recoil distance. 34Cl deduced levels, T1/2, γ-branching.

doi: 10.1103/PhysRevC.4.398
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1970CO28      Phys.Lett. 33B, 297 (1970)

S.Cochavi, J.M.McDonald, D.B.Fossan

The Magnetic Moment of the 2761 keV 8+ State in 92Mo

NUCLEAR REACTIONS 90Zr(α, 2nγ), E=24 MeV; measured nγ(θ, H, t). 92Mo level deduced g.

doi: 10.1016/0370-2693(70)90274-1
Citations: PlumX Metrics


1970MA07      Nucl.Phys. A142, 263 (1970)

S.G.Malmskog, J.McDonald

The 93.54 keV Level in 91Sr

RADIOACTIVITY 91Rb[from 235U fission]; measured Eγ, Iγ, I(ce), βce-delay. 91Sr deduced levels, T1/2, J, π, ICC, γ-multipolarities, γ-mixing. Isotopically separated source, Ge(Li) singles, electron lens coin spectrometer.

doi: 10.1016/0375-9474(70)90528-2
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1968MC04      Nucl.Phys. A109, 529 (1968)

J.McDonald, D.Porter

Excited States in 111Cd

RADIOACTIVITY 111Ag [from 110Pd(n, γ)]; measured βγ-delay, Eγ. 111Cd level deduced T1/2. Enriched target, Ge(Li) detector. 111Cd(α, α'γ), E=8 MeV; measured σ(Eγ). 111Cd deduced levels, B(E2), T1/2. Enriched target, Ge(Li) detector.

doi: 10.1016/0375-9474(68)90025-0
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1967MC13      Nucl.Phys. A104, 177 (1967)

J.McDonald, D.Porter, D.T.Stewart

Excited States in 115In

RADIOACTIVITY 115Cd [from 114Cd(n, γ)]; measured Iγ, I(X-ray), βγ-, γγ-delay, ICC. 115In deduced T1/2, multipolarity. Enriched target, Si(Li) detector. 115In(α, α'γ), E=8 MeV; 115In(16O, 16O'γ), E=35 MeV; measured σ(Eγ). 115In deduced level, B(E2). Natural target, Ge(Li) detector.

doi: 10.1016/0375-9474(67)90762-2
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Note: The following list of authors and aliases matches the search parameter J.McDonald: , J.E.MCDONALD, J.L.MCDONALD, J.M.MCDONALD, J.S.MCDONALD, J.W.MCDONALD